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Spontaneously excited magnetic fields can produce cross-field transport of the polaritons at quantum scales.
This means that a cross-field electric field is produced by the dynamo effect of the cross-field particle drift or acceleration due to electrostatic waves.
In realistic situations, the cross-field electric field is determined by the magnetohydrodynamic equations, including the cross-field particle drift given by (17) and (18).
Simultaneously, a transverse electric field can be created in the laboratory system via the dynamo effect due to cross-field particle acceleration.
In the present case, the azimuthal dependence (cgs\c 0) must be retained, since the unperturbed momentum distribution function includes the cross-field particle drift.
This leads to anomalous cross-field electron thermal transport.
Intuitively, it becomes easier for cross-field currents to flow, because they can flow across the thin direction of the fans.
In these codes, anomalous cross-field plasma transport is usually described by adding diffusive terms into the particle and energy balance equations.
Despite these difficulties, some discussion is included below of how the conclusions of the present study compare to those of the cross-field comparison.
The process of resonant absorption, and the related phenomenon of phase mixing, may occur in magnetofluids when there is a cross-field inhomogeneity.
This infinitesimal crossfield particle drift generates simultaneously an infinitesimal cross-field electric field given by (7) via its dynamo effect.
A first-order quasiparticle invariant has been presented, and the adiabatic invariance of the kinetic energy of cross-field particle motion has been explained.
Accordingly, a further theoretical investigation of relativistic cross-field particle acceleration due to electromagnetic waves should be performed.
In order to come close to these requirements, impurity injection into the edge plasma in the cross-field direction can be used.
There are up to six pits per cross-field; these show an inclined oval aperture.
